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Quark confinement mechanism and QCD phase transition 1.Conefinement by Density-de pendent quark masses (CDD M) 2.Comparison with the bag me chanism 3. EoS of quark matter in C DDM 4. EoS of nuclear matter in Bre GUCAS & IHEP, Chinese Academy of Sciences National Natural Science Foundation Committee of China G.X.Peng 彭彭彭 [email protected]. cn RC 77(2008)065807; 72(2005)015204; 62(2000)025801; 61(2000) 0

Quark confinement mechanism and QCD phase transition

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Quark confinement mechanism and QCD phase transition. G.X.Peng 彭光雄 [email protected]. GUCAS & IHEP, Chinese Academy of Sciences. National Natural Science Foundation Committee of China. Conefinement by Density-dependent quark masses (CDDM) Comparison with the bag mechanism - PowerPoint PPT Presentation

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Page 1: Quark confinement mechanism and QCD phase transition

Quark confinement mechanism and QCD phase transition

1. Conefinement by Density-dependent quark masses (CDDM)

2. Comparison with the bag mechanism3. EoS of quark matter in CDDM4. EoS of nuclear matter in Breuckner theory

4. Some preliminary results

GUCAS & IHEP, Chinese Academy of SciencesNational Natural Science Foundation Committee of China

G.X.Peng 彭光雄 [email protected]

Ref: PRC 77(2008)065807; 72(2005)015204; 62(2000)025801; 61(2000) 015201

Page 2: Quark confinement mechanism and QCD phase transition

More stable: nuclear or quark matter?

Page 3: Quark confinement mechanism and QCD phase transition

Quark confinement mechanism

MIT bag

CDDM

Page 4: Quark confinement mechanism and QCD phase transition

Drawback of bag model (I)

Sound velosity not zero for massless quarks

Page 5: Quark confinement mechanism and QCD phase transition

Drawback of bag model (II): EoS always concave

Page 6: Quark confinement mechanism and QCD phase transition

Confinement by density-dependent quark masses

CDDM

Page 7: Quark confinement mechanism and QCD phase transition

History

1. Fowler, Raha, Weiner suggested

Z. Phys. C 9 (1981) 271

2. Chakrabarty, Raha, Sinha extended it to include strange quarks

Phys. Lett. B 229 (1989) 112Phys. Rev. D 43 (1991) 627; 48 (1993) 1409

Europhys. Lett. 56 (2001) 361; Phys. Rev. C 67 (2003) 015202.

3. Zhang and Su et. al. extended it to include temperature

Page 8: Quark confinement mechanism and QCD phase transition

Main weakpoints of the previous treatment

PRD 51 (1995) 1989, PRD 52 (1995) 1276

1. The quark mass scaling is not derived2. The vacuum limits are incorrect3. There are thermodynamic problems

Page 9: Quark confinement mechanism and QCD phase transition

Confinement by density-dependent quark masses

Page 10: Quark confinement mechanism and QCD phase transition

Quark mass scaling

Page 11: Quark confinement mechanism and QCD phase transition

Quark mass scaling

Z=1/3, T=150—170 MeV

Page 12: Quark confinement mechanism and QCD phase transition

Thermodynamic consistency

Peng et al, PRC 77 (2008) 065807

Page 13: Quark confinement mechanism and QCD phase transition

Schematic comparison (I)

Page 14: Quark confinement mechanism and QCD phase transition

Schematic comparison (II)

Page 15: Quark confinement mechanism and QCD phase transition

EoS of quark matter at finite density and temperature

Page 16: Quark confinement mechanism and QCD phase transition

Transition from nuclear to quark matter (II)

nm qm

Page 17: Quark confinement mechanism and QCD phase transition

Gibbs Conditions 吉布斯条件

Page 18: Quark confinement mechanism and QCD phase transition

Conservations 守衡律

1. Electric charge

2. Baryon number

=0

Page 19: Quark confinement mechanism and QCD phase transition

Nuclear EOS in the Brueckner theory with three-body forces

Page 20: Quark confinement mechanism and QCD phase transition

The pressure

Page 21: Quark confinement mechanism and QCD phase transition

The energy density

Page 22: Quark confinement mechanism and QCD phase transition

Phase diagram at zero temperature

Page 23: Quark confinement mechanism and QCD phase transition

Structure of compact stars

Page 24: Quark confinement mechanism and QCD phase transition

道可道,非常道,名可名,非常名。无名,天地之始;有名,万物之母。故常无,欲以观其妙;常有,欲以观其徼。此两者,同出而异名,同谓之玄;玄之又玄,众妙之门。

Critical densities for given proton fractions

Page 25: Quark confinement mechanism and QCD phase transition

道可道,非常道,名可名,非常名。无名,天地之始;有名,万物之母。故常无,欲以观其妙;常有,欲以观其徼。此两者,同出而异名,同谓之玄;玄之又玄,众妙之门。

Isentropic evolution of QGP

Page 26: Quark confinement mechanism and QCD phase transition

道可道,非常道,名可名,非常名。无名,天地之始;有名,万物之母。故常无,欲以观其妙;常有,欲以观其徼。此两者,同出而异名,同谓之玄;玄之又玄,众妙之门。

Properties of strangelets

Page 27: Quark confinement mechanism and QCD phase transition

道可道,非常道,名可名,非常名。无名,天地之始;有名,万物之母。故常无,欲以观其妙;常有,欲以观其徼。此两者,同出而异名,同谓之玄;玄之又玄,众妙之门。

Summary

We have provided a new approach toconsider quark confinement. It is appliedto investigating the QCD Phase transition, the evolution of a QGO, the stractureof compact stars, and prperties ofstrangelets, etc.

Page 28: Quark confinement mechanism and QCD phase transition
Page 29: Quark confinement mechanism and QCD phase transition